ECE 340 Lecture 14 : Carrier R-G II

ECE 340Lecture 14 : Carrier R-G II

Class Outline:

•Direct Recombination•Steady State Carrier Generation

• What are the major mechanisms for recombination?

• What are the major mechanisms for generation?

• What is trapping?• How do I describe the carrier

concentrations out of equilibrium?M. J. Gilbert ECE 340 – Lecture 1 4 09/23/1 1

Things you should know when you leave…

Key Questions

M. J. Gilbert ECE 340 – Lecture 1 4 09/23/1 1

Direct RecombinationIf a beam of photons hits a semiconductor, there should be some predictable amount of absorption…This should depend on materials parameters:•Thickness•Energy of photons

Monochromator DetectorI0 IT

•A beam of photons (photons/cm2*s) is directed at the sample of thickness, l, where the beam only contains photons of wavelength, λ. •The intensity of the transmitted beam can be calculated by considering the absorption in any increment dx.•Since the photon has no memory of how far it has travelled, the probability of absorption is constant.

( ) ( )xIdx

xdI α=− Degradation of intensity is proportional to the intensity remaining at x.


Direct RecombinationThis equation is easy to solve…

Monochromator DetectorI0 IT

( ) xeIxI α−= 0

• α is the absorption coefficient and has units of cm-1.

• There is negligible absorption at long wavelengths (hν small) and considerable absorption of photons with energies greater than EG.


Direct RecombinationDepending on the bandstructure, electrons may recombine directly or indirectly…•Direct recombination occurs spontaneously – constant in time.•Decay of excess carriers should be exponential.•Decay of electrons is proportional to the number of electrons and holes remaining at time t and a proportionality constant for recombination, αr.

200 irri npng αα ==

But we want the net rate of change in the conduction band electron concentration… ( ) ( ) ( )tptnn

dttdn

rir αα −= 2Thermal generation rate

Recombination rate

Let’s make some assumptions:1. Excess e-h pairs created by

short flash of light.2. Initial electron and hole

concentrations are equal.3. They recombine at an equal

rate. (δn = δp)

Rewrite this in terms of equilibrium n and p and excess n and p…

( ) ( )[ ] ( )[ ]

( ) ( ) ( )[ ]tntnpn

tpptnnndt

tnd

r

rir

200

002

δδα

δδααδ

++−=

++−=


Direct RecombinationThis equation is hard to solve, let’s simplify…

( ) ( )[ ] ( )[ ]

( ) ( ) ( )[ ]tntnpn

tpptnnndt

tnd

r

rir

200

002

δδα

δδααδ

++−=

++−=•Assume low level injection and a small amount of excess carriers.•Assume the material is extrinsic (p-type).

Now we can easily solve this equation… ( ) nr

ttp nenetn ταδ

−− ∆=∆= 0

Where we define the recombination lifetime, or minority carrier lifetime…

0

0

1

1

n

p

np

nn

ατ

ατ

=

=

( )00

1pnn

n +=α

τor

•Excess majority carriers decay at same rate as minority carriers.•There is a large change in the minority carrier concentration, but a small one in the majority carrier concentration.


Direct RecombinationLet’s visualize this decay of carriers…

• This sample is doped with 1015 cm-3 acceptor atoms.

• The intrinsic carrier concentration is about 106

cm-3 in GaAs.• Minority carrier

concentration is ~ 103 cm-3.• 1014 cm-3 EHP are added to

the system.• Figure shows the decay

lifetime of the excess populations for a carrier recombination lifetime of 10 ns.


Steady State Carrier GenerationWe have been discussing carrier recombination…

Type 1: Direct recombination•Electron and hole drift into the same vicinity and recombine.•They can give off light if the semiconductor has a direct bandgap.

Type 2: R-G Center recombination•R-G centers may be impurity atoms or lattice defects.•Create states in the band gap.•Electrons see a potential well and get trapped losing energy. Holes are attracted to the electron and annihilates it giving off heat to the lattice.

Type 3: Auger recombination•Collision between two like carriers.•Energy released by recombination is given to the surviving carrier.•Surviving electron then loses excess energy through lattice collisions.


Steady State Carrier GenerationBut where there is recombination, there is generation…

Type 1: Band-band generation•Electron is excited directly from the valence band to the conduction band.•Either thermal energy or light can provide the energy required for the transition.

Type 2: R-G Center generation•Create states in the band gap as in the case of recombination.•Electrons absorb phonons and are excited from the valence band to the impurity band. A second phonon interaction promotes the electron into the conduction band

Type 3: Impact ionization generation•Occurs in high electric field regions.•Electrons gain enough energy that when they collide with the lattice they ionize and electron and create an electron-hole pair.•Created electrons are then accelerated and the process repeats.


Steady State Carrier GenerationIn the steady state…

• The generation rate must be balanced by the recombination rate.

• Further, this equality maintains the equilibrium carrier concentrations and must include all possible generation mechanisms.

=

20000 inpnRG =⇒= inpnpn ==⇒= 0000

Thermal generation rate


Steady State Carrier GenerationNow let’s shine light on the situation…We must now add an additional generation rate (gop) to the generation process…

•Carrier concentrations n and p will increase to new steady state values.

•We can express the balance between carrier recombination and generation in terms of the equilibrium carrier concentrations and the departures from equilibrium…


Steady State Carrier Generation What are we neglecting?

•Probability of direct electron-hole recombination in group IV materials is very small.•Recombination events occur through traps.•Energy given off as heat rather than light.

a) Incoming photon is absorbed creating an EHP.

b) Electron interacts with the lattice until it reaches the bottom of the conduction band.

c) Electron is trapped by impurity level Eiand continues to be trapped until it is re-excited to the conduction band.

d) Direct recombination occurs


Steady State Carrier GenerationSo we ignore trapping…

For steady state recombination δn = δp, so we now have…

Thermal generation rate

Assume again that we have low-level injection so we can neglect the δn2 term…

0

0

1

1

n

p

np

nn

ατ

ατ

=

=And the excess carrier concentration may be written as…

Caution: when trapping is present these rates for electrons and holes are not equal…


Steady State Carrier GenerationBut we’re not in equilibrium, so what happens now??

TkEE

i

TkEE

i

b

fi

b

if

enp

enn−

−

=

=When we were in equilibrium…

Carrier concentrations have a one-one correspondence with the Fermi level.

Consider the following situation: a uniformly donor doped silicon wafer maintained at room temperature is suddenly illuminated with light at time t = 0. Assuming ND = 1015 cm-3, τp = 10-6 sec and a light induced creation of 1017 electrons and holes per cm3-sec throughout the semiconductor.

How do we describe the bands, carrier concentrations, diffusion currents?


Steady State Carrier GenerationLet’s examine what happens when t >> τp…

The excess carrier concentration is: 21110 −==∆ cmgp popn τ

The carrier concentrations then become… 3150

3110

10

10−

−

=≅

=∆+=

cmnncmppp

Old Band Diagram New Band Diagram

•The electron concentration is unperturbed but the hole concentration has increased many orders of magnitude.•The old band diagram no longer adequately represents the situation in the semiconductor as the Fermi level is only defined for a system in equilibrium.•To deduce the carrier concentrations, we introduce the quasi-fermi levels.


Steady State Carrier GenerationHow do we get the carrier concentrations from the quasi-fermi levels?

Electron quasi-fermi level:

Hole quasi-fermi level:

• We can now use the same formalism to determine the carrier concentrations out of equilibrium.

• The above equations are assuming that the semiconductor is non-degenerate.

• Notice that FN and FP are simply conceptual constructs determined by prior knowledge of n and p.

• The quasi-fermi levels are chosen so that if the system relaxes back to equilibrium then normal carrier concentration equations are recovered.

ECE 340 Lecture 14 : Carrier R-G II

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